The type of magnetic order induced in local moments by a Kitaev-type spin liquid is controlled by whether the spin operators commute with the spin liquid's flux operators, yielding short-range Kitaev, long-range RKKY-like, or dimerized phases.
Microscopic Roadmap to a Yao-Lee Spin-Orbital Liquid
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abstract
The exactly solvable spin-1/2 Kitaev model on a honeycomb lattice has drawn significant interest, as it offers a pathway to realizing the long-sought after quantum spin liquid. Building upon the Kitaev model, Yao and Lee introduced another exactly solvable model on an unusual star lattice featuring non-abelian spinons. The additional pseudospin degrees of freedom in this model could provide greater stability against perturbations, making this model appealing. However, a mechanism to realize such an interaction in a standard honeycomb lattice remains unknown. Here we provide a microscopic theory to obtain the Yao-Lee model on a honeycomb lattice by utilizing strong spin-orbit coupling of anions edge-shared between two $e_g$ ions in the exchange processes. This mechanism leads to the desired bond-dependent interaction among spins rather than orbitals, unique to our model, implying that the orbitals fractionalize into gapless Majorana fermions and fermionic octupolar excitations emerge. Since the conventional Kugel-Khomskii interaction also appears, we examine the phase diagram including these interactions using classical Monte Carlo simulations and exact diagonalization techniques. Our findings reveal a broad region of disordered states that break rotational symmetry in the bond energy, suggesting intriguing behavior reminiscent of a spin-orbital liquid.
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Magnetic order through Kondo coupling to quantum spin liquids
The type of magnetic order induced in local moments by a Kitaev-type spin liquid is controlled by whether the spin operators commute with the spin liquid's flux operators, yielding short-range Kitaev, long-range RKKY-like, or dimerized phases.